Transient analyzing system



Jan. 12, 1954 D. E. MAXWELL 2 ,17

TRANSIENT ANALYZING SYSTEM Filed Oct. 29, 1948 ZR WI/W W Svs TEM 1/6 6 Sheets-Sheet l 4 To BE TESTED ,2 I

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I INVENTOR DONALD E. MAXWELL ATTORNE 5 Jan. 12, 1954 D. E. MAXWELL 2,666,179

TRANSIENT ANALYZING SYSTEM Filed 001;. 29, 1948 6 Sheer.sShee 1 2 AA A A A A A A A A A vvvvvv J v v v 7' v v v I l B A A A l A l A l A A A A A A A A A A INVENTORI DONALD E. MAXWELL ATTO R EYS Filed Oct. 29, 1948 Jan. 12, 1954 D. E. MAXWELL 2,666,179

TRANSIENT ANALYZING SYSTEM 6 Sheets-Sheet 3 I A iza Z4 25 Wim W m 42 gl 2/ 45 74 w 1 ;21 m f 2w I k v 54 2M 56 62 i C H m 64- I I F M L. '.i. z i 1 .i [IN/V214 72 AW l l 2/? w V l I I 74 1 r8 76 VW Q L J INVENTOR DONALD E. MAXWELL ATTOR EYS Jan. 12, 1954 D. E. MAXWELL TRANSIENT ANALYZING SYSTEM 6 Sheets-Sheet 4 Filed Oct. 29, 1948 INVENTOR DONALD E. MAXWELL 4.1% ATTORNE S Jan. 12, 1954 D. E. MAXWELL TRANSIENT ANALYZING SYSTEM 6 Sheets-Sheet 5 Filed Oct. 29, 1948 INVENTOR DONALD MAXWELL ATTORNE S D. E. MAXWELL TRANSIENT ANALYZING SYSTEM Jan. 12, 1954 6 Sheets-Sheet 5 Filed Oct. 29, 1948 INVENTOR DONALD E. MAXWELL Patented Jan. 12, 1954 y UNITED STATES i?ATENT OFFICE TRANSIENT ANALYZING SYSTEM.

DonaldE. Maxwell, New Canaan, Conn assignor to General Electric Company, a corporation of New York Application October 29, 1948, Serial No. 57,215

7 Claims. (01. 324-57) This invention relates to the measurement of original level; the display being synchronized so transient characteristics. More particularly, it as to maintain a steady pattern that may be relates to systems for the precise analysis of the studied or photographed as desired. transient characteristics of many types of audio Accordingly, it is an object of this: invention frequency andacoustic devices. 5 to provide an improved system for studying In the design or study of apparatus for amplitransient or dynamic characteristics of wavefying, recording, reproducing, or handling audio handling apparatus. frequency signals, much canbe learned of the Another object is to provide such a system havcharacteristics of the equipment by testing the ing an improved arrangement for displaying such apparatus with sine waves, the frequency of transient characteristics. which may be varied throughout the audio spec- Still another object is to provide improved trum. However, apparatus that appears to be methods and apparatus for synchronizing the satisfactory from the results of such measurevisual display of such phenomena. ments may have other characteristics that are Another object is to provide such a system havundesirable. For example, whenthe audio level, ing an improved synchronized system for obthat is, the magnitude of the signals, suddenly taining the desiredflrapid' amplitude change.

changes from a low to a higher levelthere may Anotherobject is to provide an improved balbe momentary reactions within the apparatus ancing circuit for eliminating thump or other. which prevent faithful reproduction of the sound. undesired signal'components. One method of measuring this eifect is to apply A further object is to provide improved comsquare waves to the apparatus, but this procedure p-onents; circuit arrangements, and methods s h S Va e that is diiiicult toanalyz which form only a part of the entire measuring the results. system, but which in themselves are novel and The present invention provides for a somewhat useful in other applications. different measuring technique, utilizing the sine Other objects will be in part pointed out in Waves of. changing amplitudes, and includes an th f ll i d c i ti d i part apnarent electronic system for visually presenting the refrom consideration of that description in consults of the test. This system is useful in the ne ti n ith the accompanying drawings in study of the transient responses of audio frewhich: quency amplifiers, microphones, loudspeakers, Fig. l isa block diagram of the apparatus for and other audio frequency and acoustical destudying transient or dynamic characteristics of vices, and can be utilized also to investigate the an audio frequency device or system; acoustical buildup and decay characteristics of Fig. 2 shows the instantaneous time relationreverberent structures such as concert halls and ships between the signals occurring at various broadcasting studios. points within thesystem;

In accordance with one aspect of the present Fig. 3 is a block diagram of the electronic invention, a sine wave voltage is applied to the switch and synchronizer unit; input circuit of the device or system to be meas- Figs. 4, 5 and 6 are circuit diagrams of the ured, then at a subsequent time the amplitude electronic switch and, synchronizer unit; of this signal is caused to increase rapidly to a Fig. 7 illustrates the acoustic wave form resultlarger value, maintained at this value for a cering from the'application of a test signal a typical tain interval and then restored to its origt o-unit loudspeaker. inal magnitude. Provision is made for syn- Fig s howsthe acoustic output of a typical chronization of a cathode ray oscilloscope so that single-unit type of' loud speaker such as is found theoutput signal of the apparatus under test can in home radio receivers; and be observed Visually o P g aphed. Ina ple- Fig. 9 illustrates the electrical voltage applied ferred embodiment, the visual display includes a to a loud speaker in a typical large broadcast stue few cycles of the sine Wave of the output signal dig-together with the ave form pickedup by a volt bef r the inc e in m de, the microphone positioned at some distance from the tirei'signal. during. the increased magnitude, and m d-s eaker; a few cycles"aftenthereturn'of:the=signal to its The block diagram of Fig. 1 illustrates the 3 operatic of a preferred embodiment of the sysa frequency signal generator 2 provides initial test signal 2A (corresponding to curve A -n Fig. 2), advantageously is variable over the audio frequency range, say, from 50 to 15,390 cycles. The signal BA from the si nal generator 2 is applied to an electronic switch synchrcnizer 1 nit d, which erforrns two principal functions: (1) It recurrently increases the amplitude of the audio signal 2A from genorator 2, causing this sudden increase in amplitude to take place at the exact time when the signal 2A is crossing the zero-axis. After a certain number of cycles, the signal is reduced to its lower value, thus forming a signal 2R (curve R in Fig. 2) that is applied to the input of an audio frequency system 6, the audio characteristics of wl'iich are bei lg investigated. (2) The electronic switch and synchronizer unit 3 also provides a series of synchronizing pulses 2K, which may or ma not be spaced exactly uniformly as a function of time, but which bear an exact predetermined time relationship to the high amplitude signals" of signal 28,. Thes pulses advantageously are arranged to occur a few cycles before the increase in amplitude of signal 2B and are applied to the external synchronizing terminal 7 of an oscilloscope 8 order to start the sweep of the oscilloscope so as to ive the most desirable display of the transient or dynamic characteristics of the audio system a. The output signal from the audio system c is applied to the vertical deflection terminal 5 of the cathode ray oscilloscope 8 in the usual manner.

It is apparent that for many applications the pulse-duration of the signal 2R, that is, the time during which the applied sine waves have increased amplitude, may be relatively short as compared with th intervals between the pulse for example, in testing a loud speaker, it may be desirable to use a thousand cycle signal with a pulse-duration of 10 milliseconds (ten cycles of the sine wave voltage) and to provide an interval between successive pulses of approximately one second. The problem of synchronization is immediately apparent; that is, the increased amplitude advantageously occurs at the exact instant when the sine wave is crossing the zeroaxis, thus necessitating an internal synchronization system within the electronic switch and synchronizing unit 3. The problem is further complicated by the fact that it is desirable in a practical unit that the audio frequency be continucusly variable and that both the pulse length and the repetition rate of the signal 2R- be independently adjustable. Moreover, suitable external synchronising signals must be provided in order that a stationary pattern will be obtained upon the oscilloscope or other indicating or recording device.

An understanding of the operation of the electronic switch and synchronizer unit d can be obtained by considering the curves shown in Fig. 2, together with the block diagram of Fig. 3. The signal generator which may be a standard type audio oscillator delivers a sine wave voltage of the desired frequency to terminals E2 of the electronic switch and synchronizer unit 4 (Fig. 3) The wave forms appearing in the block diagram of Fig. 3 are appropriately lettered to correspond to the wave forms having similar alphabetical designations in Fig. 2, where they are presented on a common time axis. The signal from input terminals it is divided, and part of the signal is applied to an electronic switch, generally indicated at it, and part applied to a synchronizer and switching-pulse generator, generally indicated at it.

To control the action of the latter unit, the input signal is applied to a manually variable phase-shift network ill, by which the phase may be shifted as desired throughout 360 degrees. This phase shifting network is utilized in adjusting the equipment so that the amplitude change will occur exactly at the time when the input signal 2A is crossing the zero axis.

The sine wave 213 from the phase-shift network [8 is identical with the input signal 2A, except that it is shifted in phase With respect to signal 2A. This signal is applied to an amplifier and squaring stage 22, which includes suitable means for clipping the positive and negative peaks to produce a square wave signal 2C,

the magnitude of which is adjustable by means of a potentiometer This square wave is in phase with the sine wave signal 213 from which it is derived. The square wave signal 2C is applied to a gating stage it, which is controlled by the output of a free-running, dissymrnetrical multivibrator 28 which delivers the wave form 2D, the dissyininetry of which is adjustable by means of a variable resistor 32 so that the time Tb (see Fig. 213) can be varied, for example, between the limits of approximately 0.3 second and 3 seconds. In this example, the time To (also indicated in Fig. 2D) remains fixed at approximately .015 second for all values of Tb. A suitable switch is provided in connection with multivibrator 23 to convert it from a free-running type to a biased one-shot type so that the mul tivibrator will operate for only one cycle whenever suitable initiating voltage is applied. This is equivalent to increasing the time Tb to infinity.

The signal from multivibrator 28 (Fig. 3) controls the operation of gating stage 25 and permits the passage only of negative portions of the square wave 2C, and permits these portions to pass only during the time Ta, to produce the wave form 2F.

For successful operation of the electronic switch and synchronizer unit, it is required that there be synchronism between the random pulsing of the multivibrator lit and the applied sine wave voltage 2A from the eaternal signal generator. Because the multivibrator in many applications will be recycling at a very slow rate, for example, once every three seconds, and because the applied sine wave frequency may be as high as 15,600 cycles per second, synchronization by any of the usual methods would be exceedingly compleX and difficult of adjustment. The synchro nizing system to be described is relatively simple and, once adjusted for a given sine wave frequency is independent of the recycling rate or multivibrator 28. Synchronization is assured by this system for even a single random cycle of the multivibrator, as would occur in one-shot operation. This synchronization is effected by the circuits now to be described.

The gating stage 2% is arranged to operate as acoincidence circuit, that is, the bias voltages in this stage are arranged so that the voltage pulses of wave form 22) in themselves produce no output from the gating stage 26, and the signal 20 applied to the input of gating stage 25 is also of insuiiicient amplitude to cause any signal output; thus, if either the signal 20, from squaring stage or" the signal 2D; from: the multivibrator 28; isxapplied aloneto the gatingstage. 28; no out-s put signal results; However; the periodic com:- bination of'the square wave voltage ZGand the. multivibratoroutput Voltage 213: at the input of gating 2 8 producesa net output voltage during those times when Wave form: ZD isnegative, resultinginthe' wave form 2E. Note that the negative pulses fromthe multivibrator canbe of" an entirely random nature as it regards either or both of the times Ta and Te, and that no synchronism is required between the multivibrator ZB andthesQuare wave voltages 20 applied toithe gating stage 26. Thus; the time relations ship Of'the square wave pulses 2C with respect to theleading and trailing edges of the gating pulse from-the rnultivibrator 28 is not'fiired, and the'gated Wave form EFrn-ay diiier between two successive cycles of the multivibrator as shown by comparing the two pulse groups of Fig. 2F; Becauseof this lack of synchronism, the first negativepulse of "each of these groups may occur at any time from zero to one-half the period ofthe audio waveZBafter the start of each nega tive pulseoi signal 21), and the same condition applies also to the last negative pulse of each group. However, a basis for synchronization is present in that the time -measured from the trailing edgeofthefirst negative pulse of each group in' waveform 2F toeither the lead ng or trailing edge of anysubsequent negativepulse-of the same group, is exactly the same in every group.

Inorder to establish multivibrator pulses having a precise synchront'ed relationship with the sine wave signals the signal 21 is passed through a differentiating network (Fig. 3) which produces a sharp negative pulse each time the 'voltage of the'square wave signal 25 changes value in a negative direction, and-produces a similar; but.pcsitive pulse, each time the square wave voltages increases in apositive direction, thus, generating the signal 2G.

These diiierentiated pulses are utilized to control a multivibrator 38, the first positive going pulse initiating themultivibrator pulse, with the subsequent positive pulses or pips having no appreciable effect on thecircuit. However, by

ieans of a suitable time constant circuit or pipcounting circuit, any desired negative (for example, up to approximately thetenth after the Y positive initiating pip) can be made to turn the multivibrator off, thus, ending the negative multivibrator pulse of voltage created at the output of the muitivibrator 3S. this the multivibrator prevented from further operation until the succession of pipe forming one group of wave form tGhas ended, and the multivibrator will not recycle until the next group of pips ar rives ata time-Tslater'. In thisexample; the first positive pip of each group of the signal Fig. 2G initiates the multivibrator pulse, and the" third negative pip measured from the positive initiating pip endsthenegative pulse of'the multivibrator, thus, providing a basis for synchronization. It is apparent that the length To (Fig. 2) of the multivihrator pulse is exactly the same in each of thegroups and, for example; with the condition-of perfect symmetry of the square wave vcl'tag'e of wave form 20, the timeTc- Inay'correspondto an' od'dnumber of half-cycles of the sine wave voltageofwave form2B; Inthis particular example; Tcorrespondsto the period of halfcycles of 'the-sin'e-WaveZB.

The output signal from multivibrator (Fig; 3) is passed through a squaring and phase in- 6. verting: stage 42, which deliversrthe output wave forms 2H-I andiZJ; respectively.

The wave formx2J'ispassed through a diifere entiating: network 44 and: a: negative pip clipper 46 to produce the wave formZK, which. is applied to the-synchronizing-terminal. 1" (see also Fig. 1) of thecathoderayroscilloscope 8. The sweepcontrol'circuitof the oscilloscope is adapted-to pros vide a non-recurrentf sweepoof the cathode ray beam: across therscreen. of the tube upon initiation by random pulses such as those of wave form 2K; One commercial type of. oscilloscope that providesthe required type of sweep controlis the Dumont typez'l. When wave form 2K is applied toi the synchronizing circuit of such an oscillo scope, the cathode ray beam will sweep once across the screen of the tube,.starting in synchronism with each positivepulse or pip. Because each pip bears a'predetermined and synchronized phase relationship with the sine wave voltage of wave form 2A (as maybe seen from Fig. 2), it is apparent that, if. such a sine wave voltage is appliedto' the verticalldeflection circuits of the oscilloscope, the cathode ray beam will always trace exactly the same pattern on the screen for each successivescreen cycle,:thus producing a stationary pattern on the screen eventhough the interval between successive sweeps may be of a ran dom nature;

The wave forrnZH from the squaring and phase inverting stage 42 is passed through a difierenti ating network 43' and a negative pipclipper 52 toproduce' the'wave' form ZI which comprises a series of positive. pips similar tothe oscilloscope synchronizing'pulses 2K, except that. the pips of wave form 2I occur at a time To later than those of='wave form 2K.

The wave form 21: is utilized to control a one shottype multivibrator'M, each positive pulse of waveform 2I initiatinga. negative pulse by the multivibrator 54; the duration of this negative pulse being controlled by the time constants incorp orated. in the .multivibrator 54, toproduce the wave form 2M. For the purposes of visual analysis, as presented by the present system, the pulse-timeTc (see-Fig. 2) of wave form 2M need not bear a precisely fixed time duration with respectof Td'f of a successive cycleof the n1u1tivihrator 54, and, accordingly, no synchronisrn of the trailingedgeofithe negative pulses has been provided; During the-time interval between successive pips of thewave form 21, the switching pulsemultivibrator 54 is arranged to become completely quiescent, andthus is prepared for the next cycle of its operation.

Thewave form- 2M is applied to a switching, pulse-shaping, and: phase-inverting stage 55; which removeszthe characteristic negative spike on the leading edge of the wave form 2M and acts asaphase inverter to produce the wave form 2N, the. magnitude. of which is adiustable by means of a potentiometer 58.. Suitable, bias volte ages are generated by a conventional power supply 62 and are applieclthrough a potentiometer control lidandstage 56,. to regulate the operation of switching unit M.

The signal 2N is utilized to control the switchingactionofthe electronic switch M. As mentionedabove, the'input signal from terminals I2 is applied to the electronic switch It, the signal being: applied through i a balanced low-impedance attenuator 66 to the primary of an audio transformer 68, the secondary of which is connected to the control grids'of push-pull switching stages 12 and 'l'd During the positive pulses of wave form 2N, the transconductance of the tubes in stages 12 and 14 is increased by an amount depending upon the adjustment of control 58. Thus, stage 12 produces the wave form 2P and stage it produces the Wave form 2Q. These wave forms are combined in a balancing stage [6 to produce the final wave form 2B the magnitude of which may be controlled by a potentiometer 18. The signal 215?, is applied to the input of the apparatus to be tested and utilized as described above.

The phase relationships of the various signals generated within the system are apparent from an examination of Fig. 2. Thus, for example, it will be seen that the increase in amplitude of the signal 2R, at points 82, always occurs at a time when the signal is crossing the zero axis. This is because the signal 2N, which controls the switching action, maintains a predetermined synchronized relationship with signal 213. The signal 213 is adjustable in phase bymeans of the phase-adjuster I8 throughout 360 degrees so that it is apparent that adjustment of this control will produce the desired condition under all conditions of operation.

In this particular example, it is apparent also that the synchronizing pulses 2K initiate the oscilloscope sweep at points 84 thus providing presentation of a few cycles of wave form 2R preceding the increase in amplitude occurring at points 82.

It will be apparent that the individual circuits that may be utilized to perform the functions indicated by Figs. 2 and 3 may vary widely in nature, and the following description of detailed circuits for performing these functions is illustrative of a suitable arrangement and is given for the purpose of enabling those familiar with this art to devise and adapt suitable circuit arrangements each as may be best suited to a particular application.

Sgnchronizer and switching pulse generator 16- phase shift network 18 In Figures 4, 5, and 6, underlined numerals indicate generally the detail circuits for performing the functions of the correspondingly numbered blocks in Fig. 3.

The signal 2A from the signal generator 2 is applied to the terminals 52 (Fig. 4) which are connected to a reversing switch 86 so that the phase of the input signal may be shifted 180 degrees. The output of phase reversing switch 86 is applied through a network comprising a variable resistance element 83 and a capacitor 92. Adjustment of resistor $8 provides continuous adjustment of the phase of the test voltage over a, range of approximately 180 degrees, so that, in combination with switch 36, continuous control or the phase shift throughout the 360 degree cycle is obtainable.

Sine wave amplifier, squaring, and clipping stages 22 The signal 25 from the phase shift network 58 applied to a control grid 94 of a dual triode vacuum tube t5, the left-hand section of which (as seen in Fig. 4) acts as a class A amplifier stage.

The cathode 91 of thissection of tube 96 is connected to ground through a bias resistor 98 and through a bleeder resistance 99 to a power supply, diagrammatically indicated at A, which, for example, delivers a regulated voltage of approximately 260 volts. The anode I08 of this section is connected through a plate load resistance Nil to the power supply A.

The output signal appearing at anode H30 oi this stage is applied through a condenser m2 and a resistor I03 to a control grid we of the right-hand or second section of the same tube, this section providing further amplification and peak-clipping of the sine wave resulting in a partially squared output wave form. The cathode H15 of this section is connected directly to ground, and the anode M5 is connected through a plate load resistance iii! to the power source A. Control grid ififil of the second section of dual triode is connected also through a resistance I89 to point HI, whereby a positive voltage will be applied to grid [M from a source described below. The output section of tube 95 is shunted by a dual diode clipper tube i i2 which symmetrically clips both the positive and nega tive peaks to produce a substantially square wave form 20 of the same frequency as the input wave 25. Anode Hill is coupled through a condenser H3 to anode H 1 and cathode N5 of dual diode tube H2. A positive voltage is app ied to cathode H8 of this tube, which cooperates with anode ll-i, by means of a voltage divider comprising resistances E22 and i2 3 connected in series between power source A and ground; the cathode H3 being connected between resistors I22 and I24, so that a positive bias voltage, for example, of ten volts is impressed on cathode 5 i8. The cathode i it is connected also to ground through a condenser 52% in parallel with resistor lZ t.

A suitable negative bias voltage, for example, ten volts, is applied to anode i372 of tube H2 through a lead i3 3 which connects to the bias supply generally indicated at 52 in Fig. 5.

Gating stage 26 The amplitude of the square wave at the output of tube H2 is continuously variable by means of the potentiometer 2t, and is coupled through a lead I42 to a control grid its in the second or right-hand section of a dual triode tube M5. Cathodes M8 and i52 are connected together and biased positively by meansof a voltage divider circuit comprising series resistors hi l and 56 extending between the power source A and ground. the cathodes being connected to a point between these resistors. The resistor l56 is unbypassed so that the first and second sections of tube I48 are coupled together through the common cathode circuit. The control grid I58 of the first section is connected to the output of the free-running multivibrator, generally indicated at 28.

Non-synchronous, variable repetition-rate multivibrator 28 This multivibrator which is a dissymmetrical multivibrator producing the wave form 213 comprises a dual vacuum tube I62. Control grid Hi l of the first or left-hand section is connected through a fixed resistance Hit in series with a variable resistance 32 (for adjusting the dissymmetry of the generated wave form) to arm H2 of a single pole, double throw switch, generally indicated at H3, arranged to alternatively connect resistor 32 to ground through switch area-17o contact I14 so that multivibrator I28 is freerunning and self-sustaining, or throughswitch contact I16 and lead I18 to biassupplyfilwhereby a negative voltage is placed oncontrolgrid I64 converting the multivibrator 28 into a one-shot type whereby the multivibrator operates only when it is externally initiated and then "only for one cycle. Cathodes I82 and ltd of-tube i 62 are connected directly to ground. Anode I36 of the first section is coupled through a-condenser I33 to control grid I92 ofthe second section which is provided with a D.-C. grid return through a resistance I35, which is connected to a source of positive bias applied to a lead I95 by means of a divider arrangement comprising resistors E95 and I91, connected in series between the power source A andground. (Series resistors I 93 and E99 are in parallel withresistor 591 and provide the positive bias at point HI for tube 9t. Anode 28B of the second section of tube N32 is coupled through a capacitor ZIJI to control grid its of the first section. Anodes [.86 and 2% are coupled, respectively, throughload resistors 2E2 and 28% to power sourceA.

In order to initiate the single sweep when switch arm H2 is engaged'with switch contact H3, 2. switch 2:2 is provided in series with a resistance 2M and a resistance 2H; connected in series between power source A and ground.

so that, when switch H2 is closed, a positive K Gating stage 26-continued The output signal is coupled from anode I86 through a condenser 222 to the control grid I58 of gating tube Mia, this grid being biased positively with respect to ground through a resistance 2255 connected between the grid I58 and the positive bias voltage lead I95.

With no signal applied to grid i553, the cathodes M8 and i? are at a positive potential, forexaniple, somewhat greater'than 50 volts,because of the positive bias applied to grid I58 and the resulting current iiow through the first section of the tube. Accordingly, the second section'of tube I46, in which the grid isat ll-C. ground potential, is biasedbeyond plate current cut-off. Under this condition, the square .wave voltage applied to grid M l does not cause "any plate current to flow in this section, and, thus,.no voltage appears across plateload resistor '228, which is connected between anode232 and powersource A. However, when wave form 2D from multivibrator 23 is impressed on the grid I58 of the first section of tube I46, plate current through this section is cut ofi" for the time Ta (see Fig. 2). Accordingly, the cathodes I43 and I52 become less positive, but are prevented, .by means of fixed bias, from dropping to a value which-will permit any current to flow in the second section of tube i i-i3. Thus,the voltagepulses of wave form 2D from the multivibrator 28 in themselves produce no output at the anode 2-32 of tube I46.

However, the periodic combination .of .the square wave voltage applied to grid I44 and the multivlbrator output voltage applied to grid I58 produces a net grid-cathode voltage having the wave form 3E (Fig. 2) in the second section of.

tube I46. In other words, the multivibrator pulses of wave iorm 2D, which produce no plate current flow in the second section of tube I46, in

effect, drivethe voltage 'ofthe grid -I4'4 of the second section sufiiciently positive that the positive excursionso'f the square wave voltage impressed on-this grid/cause plate current to flow in the second section. Thus, there appears across the plate load resistor 228 the discontinuous and inverted square wave shown by wave form ZF' (Fig. 2). Note,however,.that the square wave output appears across this resistance 223 only for the duration of .the time Ta (Fig. 2). Thus, the action oftube Hi6 isofa gating or coincidence nature, allowing square waves to pass only-during the negativeor gating pulsefrom the multivibrato'r 23.

As noted above, lithe negative pulses from the multivibrator may be entirely of-a random nature as regardsieitherzor l both times, .Ta and Tb, and that there is no-synchronism of any nature require'd between themultivibrator andthe square wave voltage .20 applied to the gating tube MB. Thus, the timeerelationshipaof the square wave pulses with respect ntoithe leading and trailing edges-0f thegating pulse ofthe multivibrator is not fixed,-and'the gated wave formmay differ between two successivegroups, as pointed out above and showninFig. 2E. The; gated groups of negative square wave pulses appearing at anode 232 are differentiatedbymeans or" anetwork: comprising cacapacitori23'4 andra resistance-236, connected in .series between the anode .232 and ground. The output .of this network consists ofa group of negative andtpositive voltage ilk-1 s corresponding to the'leading and trailing edges, respectivelgmof theisquarewavepulses-at the inputto the network 36. These .pipsare shown as waveform 2G:(Fig. .2). As discussed above, the timemeasured from the firstnegativepip to the first positive pip:-mayvary;from-group to group, butthe time measured fromthefirstpositivepip of 1 any group to any subsequentnegative .or positive pip-of the same group isalways exactly the samein each group,*and thus, provides a basis forsynchronization. The output of the difierentiatingnetwork 36 is applied to control grid 23-8 of a -triodevacuum tube WhlQh TOllHS a cathode-follower isolation stage. -Grid 238 is biased positively with respect to ground by means of a voltage divider arrangement comprising a resistor 242 connected in series with the resistor 236 between the powersource A and ground. .Anode 244 "of tube 240 is connected directly to power source A, and cathode 246 .of this tube is connected to ground through the cathode load re sistance 248, the output signal being taken directly from theccathocie by means oi a lead 252.

Pre-swz'tching multivibrator and phase inverter stage 38 The'signal 2G, fromtube 24B, is applied to a dual triode multivibrator tube 254 (Fig. 5) which is of the one-shot type and is controlledin operation by the signal 2G. This signal is applied, throughlead 252 and capacitor 256, to a control grid tfidof the firstsection of tube 2%; a D.-C. ground return path is provided through a resistor 262. In order to bias the first section of the tube 254 to cut-off, a voltage divider circuit is provided comprising (a resistance 264 and a resistance 266 connected in series between the power source A and ground, the cathode .268 being connected between the two 1 resistances with a suitable bypass condenser ilz connected in allel with cathode resistance Anode oi the first sectioncf tubeizii l isconnected .torthe power source A through a load resistance 27%}, and is coupled through a condenser N8 to a con trol grid :82 of the second section of tube 254. Control grid 232 is biased positively by means of a fixed resistance 284 in series with the variable resistance ii which is connected to the positive bias supply lead E95. Cathode 292 of this section is connected directly to ground. Anode 29 1 or" the second section, connected to power source A through a plate load resistance 2%, is coupled through a capacitor 298 to control grid 258 of the first section.

Thus, in the quiescent state, the first section of tube 254 is non-conducting and the second section is conducting. When Wave form 2G is applied to the first or off-section, the first pip of each group is always negative and drives the already negatively biased grid 258 still further negative, and no action occurs in the multivibrator. The first positive pip, however, renders the off-section conductive, producing a negative pulse of voltage at the output of the multivibrator 353, that is, at anode 214. Of the subsequent negative and positive pips which continue to be impressed on the grid 258, only the negative pips have any appreciable effect. These negative pips on the grid. of the first section (which is now the on-section) are inverted in the plate circuit of this section and appear as positive pips on the grid 282 of the second. of tube 254 (which is now the off-section). By suitable adjustment of the variable resistor 406, any desired negative pip (for example, up to the tenth after the positive initiating pip) appearing on the grid 258 of the first section of turn the second section of the tube back on, thus concluding the negative pulse of voltage at the output of the multivibrator, and driving the grid of the first section highly negative. Before this negative charge can leak off to the point Where a subsequent positive pip on the grid of the first section can turn this section on again, the succession of gated pips of the particular group will have ended. Therefore, the multivibrator tube 254 will not recycle until the next group of pips arrives at a time Tb later.

Squaring and phase inverting stage 42 The output wave form from multivibrator tube 25 3 is coupled from anode 2'54 through a coupling condenser 3b? to a control grid 30% of a triode tube 8%, a D.-C. ground return path being provided through a resistancet i2 which is connected to the positive bias supply lead [95.

The cathode Hit of tube 306 is connected to ground through an unbypassed cathode resistance Bit, and the anode 2H8 is connected to power source A through a plate load resistor 322. The wave form 21?: appears across the cathode resistance 3H6, while the inverted voltage, shown by wave form ZJ, appears at the anode M8. This latter voltage is passed through the differentiating network id comprising a capacitor 32d and resistance elements are and. 328 in series. These resistors 326 and 328 also perform the function of voltage division and resistance isolation. The fraction of the total difierentiated voltage'appearing across resistance 328 is shunted by the second section it of a dual diode vacuum tube 332, the cathode 33 3 of which is connected to one end of resistance 328, and the anode 33G of which is connected to the opposite end of resistance 328, that is, to ground. Thus, whenever cathode 33 becomes negative with respect to ground, current tube 254 can be made to I flows through the second section of diode 332, effectively eliminating the negative pips from lead 338, which is connected to the cathode 33s, to provide the synchronizing voltage 2K which consists of a series of positive pips corresponding 1n time with the leading edges of the pulses of the wave form 2J. These synchronizing pulses or pips are conducted by the lead 338 to output terminals are, so that it can be utilized at a positive triggering voltage for the sweep control circuit of the cathode ray oscilloscope 8.

The wave form 2H appears across cathode resistance Sit and is differentiated by means of a network 38 comprising capacitor 3-52 and resistors 3% and 3% in series, which resistors function also for the purposes of voltage division and isolation. The first section 52 of diode 332 is connected in parallel with resistance 3%, cathode ass being connected to one end of the resistor, and anode 352 to the other, or ground end, of the resistor 3%. Thus, there is developed across the resistor 348 only the positive pips which result from differentiation of the wave form 2H, producing the wave form 21 which comprises a series of positive pips corresponding in time to the trailing edges of the pulses of wave form 2H, that is, the pulses of this Wave form lag the pulses of wave form 2?: by a time corresponding to To (Fig. 2).

Switching-pulse multivibrator 54 The wave form 21 from cathode 3 38 of tube 332 is coupled through a condenser 35 i to a control grid 35E of the first section of a one-shot multivibrator tube 358, a D.-C. ground return path being provided through a resistance 3&2. This first section of the dual triode tube 358 is the off-section of the multivibrator. Cathode 364 is biased positively with respect to ground by means of a voltage divider comprising resistances 355 and 36%.. in series between power source A and ground, resistance 363 being bypassed a capacitor 3T2. Anode sis of this section is connected through plate load resistances 3'56 and 318, in series, to the power source A, and is coupled also through a capacitor 382 to a control grld 384 of the second section of tube 358. The cathode 388 of this section is connected directly to ground. The grid 38% is biased positively through a variable resistance 392 connected to the positive bias supply lead making this portion of the tube the on-section of the multivibrator. Anode 39d of this section is connected through a plate load resistance 3% to the power source A, and is coupled also through a condenser 398 back to the input grid 356 of the offsection of the tube 358. This tube thus comprises a one-shot multivibrator. When the voltage of wave form 2i is applied to the grid 356, each positive pip will initiate a pulse of negative voltage at the anode 31s as shown by curve 2M. The time duration Tu of this negative pulse is established principally by the time constant of capacitor 382 and resistance 3%. However, for the purposes of visual observation of the characteristics of peak limiting amplifiers, Ta need not bear a precisely fixed time duration with respect to T's as pointed out above, but for other applications, for example, in the analysis of acoustics phenomena, the resistance 392 can be ad- JllSted advantageously so that the time Ta corresponds to an integral multiple of the period of the sine wave 2A. During the time interval between the successive pips of wave form .521 :the switching pulse multivibrator has time; to become completely quiescent and, thus, is prepared for the next cycle of its operation.

Phase-inverting and switchi g-pulse shaping stage 56 The output voltage of the niultivibrator :tube 358 appearing at the junction of resistors .316 and did, connected to the anode 3M, is applied through a coupling condenser 402 to a controlgrid w l of the first section of a dual triode .tube Andra 11-0. ground return path being provided through a resistance 6%. The cathode 412 of this first section is returned to ground throughaca-thode resistance 3M, and anode M6 is connected to power source .A through a load resistance 418. The first section of tube Alldremovesthecharacteristic spike on the leading edgeof the wave form 2M and also acts as aphase inverterythe second section being connected as a cathode-follower which is normally biased for plate cur-rent cut-off.

Anode MS of thefirst section ofdual triodedflfi is cou led through a capacitor 322 to "a control grid 52d of the second section ofthe same tube, the grid 226 being returned to groundthrough a resistance a bias battery lz and a portion of the potentiometer 64. A suitable capacitor is connected between the positive end of battry and ground. Cathode 4350f this sect on is returned through the potentiometer 58 to the positive terminal of battery 42-3. Anode an of this section isconnected directly to the power source A. Thus, the second section of tube lilli is connected as a cathode' follower with the control grid 4% normally biased beyond plate current cut-offby the battery 428. The voltage developed across the plate-load resistor Bis coupled to the control grid 424 of thissection'and, during the time Tu, the voltage at the grid 424 is suiiiciently positive to produce plate current in the second section of tube 496. Thus, there is developed the voltage shown by wave form 2N across the cathode load potentiometer 58. A positive voltage from another battery 440 is applied also through potentiometer "64 tothe cathode 436 and to the resistors 443 and 444 which are connected in parallel therewith; a suitable condenserMt being-placed in parallel'with resistor 44 5. Lead I18 is connected to thepositive end of resistor 443, and lead I34 is connected at the junction of resistors 443 and "444,170 provide the two values of positivebias voltage for use in the circuits as described above. In order toprevent drain on the battery 441] whenthe equipment is not in use, this battery isconnected in series with a normally open switch 441, controlled by a solenoid M8, which is arranged to close switch 44? only when power source A- is energized. Thepotentiometer 4 regulates the Du-C. voltage applied to cathode 436 which voltage is used as a bias potential for the following stages, as will be described. Note, however, that because there is no plate current in the secondsection of tube 466, except duringthe time Td, there is no steady D.-C. potential developed across the *potentiometer. 58.

Electronic switching unit 14 This'signal is conducted by a lead 450 to the-midpoint of two resistors 452 and 45d which. are.connected in series with each other and in parallel with the secondary winding 456 of transformer tlltheprimary 462 of which is connected through an attenuating pad, generally indicated at 66, to the input terminals [2. The ends of secondary winding 455 are connected, respectively, to control grids 466 and lies .of super-control pentode'tubes 412 and 4M. A.D.-C. bias Voltage is applied to the grids itdand see from the batteryMiHFig. 5), the value of the bias being adjustable by means of the potentiometer 64,.and in one typical application this bias value is adjusted to a value which reduces the plate transconductance of tubes llzand 4M to a value about one-tenth of that for zero bias voltage on the grids. It is to be noticed that direct coupling has been provided between the potentiometer 5e and the grids of tubes .412 and Alain order to preserve the wave shape of the switching pulse signal ZN. Note: also that, because there is no D.C. component of volt age across the potentiometer the fixed bias on the grids 466 and Q63 is independent of the setting of this potentiometer and dependent only on the setting of potentioineter fi l.

Cathodes 476 and $78 of tubes 4112 and 4M are returned to ground through cathode resistors 482 and 48d, respectively. Anode voltage is applied to anodes 43d and 238 of these'tubes through plate load resistors Q92 and 29 respectively, which are connected to opposite ends of apotentiometer 496, the adjustable tap 598 of which is connected to the power source A. Screen grids 502 and 504 of tubes M2 and 41%, respectively, are connected together and to a source of positive voltage derived by means of a voltage divider comprising resistances 5.96 and .508 connectedbetween power source A and ground.

The positive switching pulses of wave form .ZN are of such polarity as to increase thetransconductance of the switching tubes 472 and di l during each positive pulse. Depending upon theadjustment of potentiometer 58 (Fig. 5), the-increase in transconductance during the switching pulses can be anything from zero to the order of ten times the quiescent value.

The sine wave signal voltage, from the external generator 2 that is connected to terminal I2, is applied to the tubes H2 and il l in push-pull relationship, so that the grids 366 and 468 are .degreesout of phase. However, the switching pulse IN is applied in phase-tobothtubes. Fig. 2]? shows the resulting voltage across plate load resistance 492, and Fig, 2Q represents the voltage simultaneously appearing across t-he plate load resistance't i. Note that for the duration of the switching pulse (time To) the voltages across the plate load resistors consists of a D.-C. component plus a sine wave component. The amplitude of the sine wave voltage duringithi-s switching interval is shown to be larger than during the interval between switching pulses, ibecause the increased transconductance of tubes 472 and 4141results in increasing amplification. of the sine wavevoltage.

Switching-pulse balancing stage 76 In order to remove the D.-C. component of the switching pulse from the wave forms 2P and 2Q, to produce the output wave form Fig. 2R, the signal from plate 486 is coupled through acondenser '5 l2 to a control grid 514 of the first section ofa dual triode vacuunrtubetlfi, a=D.-C.

ground return path being provided through a resistor H3, in series with a resistance 522. The signal from anode is coupled through a condenser to a control grid $26.01" the second section of dual triode tube Sit, a 11-0. return path being provided through a resistance 523 in series with the resistor 522. The cathodes 532 and 5% of this tube are connected together and to ground through a cathode resistance 53% in series with the resistor $22. This cathode resistance is unbypassed so that the first and second sections are coupled together through the common cathode resistance. The resistance 536 also provides self biasing potential for the grids of the two sections which are returned to the junction of resistors 555 and 522 through their respective grid return resistors.

Anodes 53a and 542 of this tube are connected, respectively, through resistors 54 and 5% to power source A. The plate load resistors 5M and 5% are much lower in value than the common cathode resistance formed by resistors 53% and 522.

This amplifier stage has the characteristic that the signal voltage gain from the rids 5M and '525 to either plate load resistor is very much higher for 189 degree out-oi-phase excitation of the grid than for the in-phase grid excitation. For out-of-phase (or push-pull) signal excitation, the voltage gain of tube 516 to either plate load resistor is given for practical purposes by the well known equation:

where u and Tp are identical in both sections of tube EH6, and R1. is represented by either resistor 5% or resistor 5 which, for purposes of illustration, are equal in value. However, when the grids of this tube are excited by in-phase signal voltage the voltage gain can be shown to be given by the expression:

where Re refers to the total value of resistors 522 and 53S in series. Thus, the second equation has the additional term 2(u+l)Rc appearing in the denominator. This last term can be made very large in comparison with Tp-I-RL and, accordingly, the voltage gain for in-phase excitation or the grids may be very much less than for out-of-phase excitation. By way of illustration, for the values of resistors given in the subsequent table herein and assuming tube 516 to be a type GSN'l-GT tube, Where u is 20, and Tp is 8000 ohms, the out-of-phase voltage gain to either or" the plate load resistors is approxi mately 11, whereas the in-phase voltage gain as calculated by Equation 2 is approximately 0.1, a gain reduction to in-phase voltages of 110, or 41 db.

In operation, this stage serves to remove the D.-C. component of the switching pulse from the wave forms 2P and 2Q. The wave form 2? appearing across the plate load resistance of tube ll? is applied to the control grid 5M of one section of the tube tit, and the wave form 2Q appearing across the plate load resistance of tube ll-4 is applied to the control grid 5% of the other 16 7 section of tube 51s. The sine-wave components of thesewave forms are applied to the respective grids of tube 516 in phase opposition, that is, in push-pull relationship, but the D.-C. components of the switching pulse are in-phase when applied to these grids. Accordingly, if the amplitudes of the D.C. components applied to each grid are exactly equal, the relative amplitude of the switching transient appearing across the plate load resistor will be attenuated some 41 db in comparison with the sine-wave component.

However, this arrangement is not completely satisfactory, because, to some extent at least, the switching transient is still present. In order to further reduce or completely eliminate this switching transient the potentiometer 596 is provided as a balancing control. This potentiometer permits adjustment of the total plate load resistances of tubes 432 and did to any desired degree of inequality.

In order to understand more clearly how this balancing control 496 permits complete cancellation of the switching transient, consider this circumstance: the adjustable tap 498 is in its mid-position and the total plate load of tube 472 is equal to that of tube 41 and the D.-C. component of the switching pulse appearing across the plate load resistance of tube 412 is equal to that appearing across the plate load resistance of tube di l. Under these conditions, the D.-C. component will be greatly attenuated, but will still exist in some magnitude across load-resistor 548. However, assume potentiometer 496 is now adjusted so that the switching-transient voltage applied to the grid 5M of tube tilt is slightly greater than that applied to the grid 526. This, in efiect, increases the switching transient volt age across the common cathode resistances 53B and 522, and is in the direction that tends to cancel any net transient voltage appearing between the grid 526 and cathode 5336. Accordingly, the potentiometer 396 can be adjusted to a position such that no switching transient is developed across the output plate resistor 546 of tube 516. The sine-wave component, however, is altered very little by the balancing adjustment.

It can be seen that this arrangement will permit complete elimination of the switching transient even though the switching transient from tube 312 is not equal in magnitude to that from tube di l, for example, because of individual differences in the dynamic characteristics of tubes H2 and tilt. It should be noted, moreover, that direct coupling is not required between the plate load resistances of tubes H2 and 74 and the repective grids of tube 5i 6, because it is not necessary to preserve the original square shape of the D.-C. switching component as it appears on the grids of the tube EH6, but only to retain symmetr between the two signals. Thus, capacicanoe-resistance coupling networks can be employed and the complications characteristic of direct coupling networks avoided.

The signal output voltage is coupled from anode 5t2 through a condenser 552 and variable tap 55d of the potentiometer 78 to a control grid 556 of a dual triode amplifier tube 558; the opposite end or the potentiometer 18 being connected to ground to provide a D.-C. return path. Cathode 562 of this section is connected to ground through a bias resistance 5%, and anode 565 is connected to power source A through a plate load resistor 568. Anode 566 is coupled through a condenser 5'12 to control grid 5% of the second tion of tube 558, a D.-C. return path being provided through a resistance 516. Cathode 518 of this section is connected to ground through a bias resistance 552, and anode 584 is connected to power source A through primary winding 586 of an output transformer 588. Negative feedback is provided from anode 53 through a condenser 592 and a resistor 5E4 to cathode 562. The amplifier or other apparatus to be tested is connected to secondary winding 5% of transformer 538.

The system described above is particularly applicable to the analysis of the performance of limiting amplifiers, and permits observation of the transient phenomena occurring at the output of the amplifier immediately after the application of a controlled-peak signal to the input. In such studies, it is usually desirable that the time between successive pulses be of the order of 1 to 3 seconds because the gain-recovery time of such amplifiers is ordinarily of this magnitude. In operation, the quiescent amplitude of the signal usually is adjusted to a value such that the peaklimiting amplifier is just below the point of gainreducing action. When the amplitude is suddenly increased, a gain-reducing action occurs and the time for essentially completing this action is called the "attack time of the amplifier. This gain-reducing action can be observed cycle by cycle of the applied sine wave, and the attack time can be measured b counting the number of cycles of a given frequency to the point where no further change of amplitude takes place. Accompanying aiiects, such as control-gain surges (thump) and wave form distortion are shown also with as much detail as is desired by proper adjustment of the oscilloscope sweep circuit.

It is to be noted that, with this method of transient analysis, it is important that the change in amplitude of the test signal from the lower to the higher value be made instantaneously at the time when the applied sine wave is crossing the zero axis. If the amplitude i changed during any other part of the cycle, an irregular wave front will be developed that will render the visually presented data less useful, and in many cases substantially meaningless.

In the above-described embodiment of the invention, no provision has been made for synchronizing the trailing edge of the wave form shown in Fig. 2M. However, in some applications, it may be desirable to do this, and for many applications it will be desirable to adjust the time constants of the multivibrator that produces this wave form so that precise control of the trailing edge is obtained, thus, permitting the time Ts to be adjusted to correspond to an integral multiple of the period of sine wave 2A. For use in analysis of acoustical phenomena, it is desirable that the trailing edges of the keying pulses, shown in Fig. 2M, should be sharpened, and this can be accomplished readily by means well known in the art.

Also, in acoustical analysis, and in certain other applications, it is desirable that there be no signal occurring between the successive pulses of increased amplitude of the sine wave; that is, the plate currents of tubes 472 and 414 are completely cut-oif between the successive pulses. In this case, it is desirable to utilize sharp-cut-oii tubes instead of the super-control tubes 412 and 4M. It is apparent that various other modifications may be made in the circuit details without exceeding the scope of the present invention. For example, in the above-illustrative embodiment, negative pips are used to turn off multivibrator 38, but it is apparent that the circuit could as well be arranged so that the positive pips serve as the timing control to turn off this multivibrator, the use of negative pipes probably having no other advantage than some simplification of the circuit arrangement. Such examples of equivalent arrangements could be cited at length, but it is to be understood that such substitutes are within the contemplated scope of the present invention as defined in the claims below.

The following table lists the values of the various components utilized in the above embodiment and are set forth here only for the purpose of assisting others to understand and utilize the invention and not for purposes of limitation.

Value in Thousands of Ohms Number Value in Va Microfarads esN7-GTI Figures '7, 8 and 9 show typical oscilloscope,

p esentations occurring in the use of the present system. Figure '7 shows the acoustic wave form resulting from the application of a thousand cycle signal with a 10 millisecond pulse to a typical two-unit loud speaker, the pattern indicating considerable transient distortion. Part of the irregularity of the wave form is produced because of the two acoustic signal sources involved and the difference in acoustic path between the low frequency and high frequency radiating units.

Figure 8 represents the acoustic output of a typical single unit type of loud speaker such as is ordinarily found in home receivers. In this example, the sine wave frequency is 3 kilocycles and the pulse duration is 10 milliseconds. The gradual build-up of the acoustic amplitude to a value about 10 db greater than the initial cycle, and the strong hangover, or ringing, effect after the existing voltage is removed at the end of 10 millisecond-period are readily apparent.

Figure 9 is in reality a double exposure of two separate phenomena. The pulse at the left represents the electrical voltage applied to a loud speaker in a typical large broadcast studio. The speed of the sweep circuit for this application is relatively slow. For example, 200 milliseconds in total length, so that the resolution of the loco-cycle per second signal, with a 10-mil1isecond sine wave pulse, is not shown in detail and an envelope patent results. The remainder of the oscilloscope represents the acoustic wave form picked up by a microphone positioned about 40 feet from the loud speaker, approximately 36 20 milliseconds elapses from the leading edge of the applied sine wave until the signal is received at the microphone. The relative intensities or" the direct and reflected signals are.

shown clearly. Any outstanding echo eiiect would appear as a high amplitude pip, much as a radar echo.

From the foregoing, it will be observed that the electrical apparatus embodying my invention is well adapted to attain the ends and objects hereinbefore set forth, and to be economically manufactured, because the separate components re readily obtainable as standard items here and well suited to ordinary production methods. It is apparent that the particular circuit arrangements are subject to a wide variety of modifications in accordance with the state of the art and as may be desirable in adapting the invention to different uses. it is also apparent that novel circuit arrangements utilized to perform particular functions within the system, are in themselves useful in widely varied applications, and, accordingly, these features are not intended to be limited to use with any particular combination.

What I claim is:

1. In analyzing the characteristics of wavehandling apparatus, the method comprising the steps of generating a first sine wave signal, di-

iding said signal into second and a third signals, producing a substantially square wave form having a period integrally related to the period of said second signal, generating a first control pulse having a period longer than the period of said square wave form, gating said second signal in accordance with a predetermined polarity oi said first control pulse so as to permit the passage of said square wave form only when said pulse assumes said polarity, differentiating said gated wave form to produce a series of groups of pips, generating a second control pulse synchronized with predetermined pips in each of said groups, difierentiating said second control pulse to produce synchronizing signals of low recurrence rate having a predetermined synchronized relationship with said sine wave signal, generating a third control pulse in synchronized relationship with said synchronizing signals, amplifying said sine wave signal, controlling said amplification in accordance with the characteristics of said third control pulse, passing said amplified sine wave signal through said wavehandling apparatus and coupling the output signal from said wave-handling apparatus to a visual indicator.

2. The method of analyzing the characteristics of wave-handling apparatus comprising the steps of generating a first sine wave signal, dividing said signal into second and a third signals, producing a substantially square wave form having a period integrally related to the period of said second signal, generating a first control pulse having a period longer than the period of said square wave form, gating said second termined synchronized relationship with said,

sine wave signal, generating a third control pulse in synchronized relationship with said first synchronizing signals, amplifying said sine wave signal, controlling said amplification in accordance with the characteristics of said third control pulse, passing said amplified sine wave through said wave-handling apparatus, coupling the output signal from said wave-handling apparatus to an oscilloscope, and synchronizing the sweep circuit of said oscilloscope with said second synchronizing signal.

3. Apparatus for use in measuring the characteristics .of wave-handling apparatus comprising a signal generator, an electronic switch coupled to said signal generator, a synchronizing and switching pulse generator coupled to said signal generator for controlling the action of said electronic switch, said synchronizing and switching pulse generator comprising a square wave generator actuated by the signal from said signal generator and producing a square wave hearing a predetermined synchronized relationship thereto, a gating circuit including a first pulse generator and coupled to the output of said square wave generator and selectively passing spaced groups of said square waves in accordance with the signals from said first pulse generator, a first diiferentiator circuit for differentiating said groups of square waves and producing spaced groups of control pips, a second pulse generator controlled by predetermined pips in each of said groups, a second di' ferentiator circuit coupled to said second pulse generator and producing a first and second series of spaced synchronizing pips, and a third pulse generator controlled by said first series of synchronizing pips and having an output circuit coupled to said electronic switch whereby the magnitude of the signal from said signal generator is controlled by the output of said third pulse generator, the output of said electronic switch being coupled to said wave-handling apparatus the characteristics of which are to be measured, an indicator coupled to the output of said wavehandling apparatus, and a circuit coupling said second series of synchronizing pips to said indicator.

4. Apparatus for use in measuring the characteristics of wave-handling apparatus comprising a si nal generator, a dividing circuit for dividing the signal from said signal generator into first and second parts, an adjustable phase shifter for shifting the phase of one of said parts relatively to the other, an electronic switch cou pled to said second part of said signal, a synchronizing and switching pulse generator coupled to said first part of said signal for controlling the action or said electronic switch, said synchronizing and switching pulse generator comprising a square wave generator actuated by said second part of said signal from said signal generator and producing a square wave bearing a predetermined synchronized relationship thereto, a gating circuit including a first pulse generator and coupled to the output of said square wave generator and selectively passing spaced groups of said square waves in accordance with the signals from said first pulse generator, a first difierentiator circuit for differentiating said groups of square waves and producing spaced groups of control pips, a second pulse generator controlled by predetermined pips in each of said groups, a second diiierentiator circuit coupled to said second pulse generator and producing a first and second series of spaced synchronizing pips, and a third pulse generator controlled by said first series of synchronizing pipe and having an outputcircuit coupled to said electronic switch whereby the magnitude of the signal from said signal generator is controlled by the output of said third pulse generator, the output of said electronic switch being coupled to said wavehandling apparatus the characteristics of which are to be measured, a cathode ray oscilloscope having a sweep circuit and coupled to the output of said wave-handling apparatus, and a circuit coupling said second series of synchronizing pips to said sweep circuit.

5. Apparatus for use in measuring the charaoteristics of wave-handling apparatus comprising a signal generator, a dividing circuit for dividing the signal from said generator into first and second parts, an adjustable phase shifter forshifting the phase of one of said parts relatively to the other, an electronic switch coupled to said second part of said signal, a synchronizing and switching pulse generator coupled to said first part of said signal for controlling the action of said electronic switch, said synchronising and switching pulse generator comprising a square wave generator actuated by said second part of said signal from said signal generator and producing a square wave bearing a predetermined synchronized relationship thereto, a gating circuit including a first pulse generator and coupled to the output of said square wave generator and selectively passing spaced groups of said square waves in accordance with the signals from said first pulse generator, a first differentiator circuit for differentiating said groups of square waves and producing spaced pips, a second pulse generator controlled by predetermined pips in each or said groups, a second differentiator circuit coupled to said second pulse gen rator and producing a first and second series of spaced synchronizing pips, and a third pulse generator controlled by said first series it synchronizing pips, said electronic switch comprising an amplifier for, amplifying said second part of said signal from said signal generator, a circuit coupling said third pulse generator to said amplifier whereby the gain of said amplifier caused to increase rapidly upon receipt of a pulse from said third pulse generator, said phase shifter being adjusted so that the increase in gain occurs when said second part of said signal is at substantially zero amplitude, and a balancing circuit for removing the D.-C. switching component from said amplified signal, the output of said electronic switch being coupled to said wavehandling apparatus the characteristics of which are to be measured, an indicator coupled to the output of said wave-handling apparatus, and a circuit coupling said second series of synchronizing pips to said indicator.

6. Apparatus for use in measuring the characteristics of wave-handling apparatus comprising a signal generator, an electronic switch coupled to said signal generator, a synchronizing and switching pulse generator coupled to said signal generator for controlling the action of said electronic switch, said synchronizing and switching pulse generator comprising a square wave generator actuated by the signal from. said signal generator and producing a square Wave bearing a predetermined synchronized relationship thereto, a gating circuit including a first multivibrator and coupled to the output of said square Wave generator and passing spaced groups of said square waves in accordance with the signals produced by said multivibrator, a first differentiator for differentiating said groups of square waves and producing spaced groups of control pips, a second multivibrator controlled by predetermined pips in each or said groups, a second difierentiator circuit coupled to said second multivibrator and producing a first and second series of spaced synchronizing pips, and a third multivibrator controlled by said first series of synchronizing pips, said electronic switch including two vacuum tubes arranged to handle the signal from said signal generator in pushpull manner, a circuit coupling the output of said third multivibratcr to said tubes in in-phase relationship, and a balancing circuit coupled to the output of said tubes for removing the switching component from said signals, the output of said balancing circuit being coupled to said wavehandling apparatus the characteristics of which are to be measured, an indicator coupled to the output of said wave-handling apparatus, and a circuit coupling said second series of synchronizing pips to said indicator.

7. Apparatus for use in measuring the characteristics of Wave-handling apparatus comprising a signal generator, delivering a sine wave signal, an electronic switch coupled to said signal generator, a synchronizing and switching pulse generator coupled to said signal generator for controlling the action of said electronic switch, an adjustable phase shifted for varying the relative phase of the signals coupled from said signal generator to said electronic switch and said synchronizing and switching pulse generator, said synchronizing and switching pulse generator comprising a square wave generator actuated by the signal from said signal generator and producing a square wave bearing a predetermined synchronized relationship thereto, a gating circuit including a first multivibrator and coupled to the output of said square wave generator and passing spaced groups of said square waves in accordance with the signals produced by said multivibrator, a first difierentiator for differentiating said groups of square waves and producing spaced groups of control pips, a second multivibrator controlled by predetermined pips in each of said groups and generating a series of pulses in fixed phase relationship to said sine wave signal, a second differentiator circuit coupled to said second multivibrator and producing a first and second series of spaced Synchronizing pips, and a third multivibrator controlled by said first series of synchronizing pips, said electronic switch including two amplifier tubes arranged to handle the signal from said signal generator in push-pull manner, a circuit coupling the output of said third multivibrator to said tubes in inphase relationship and controlling the amplification thereof, and a balancing circuit coupled to the output of said tubes for combining the signals therefrom and removing the switching component from the combined signals, the output of said balancing circuit being coupled to said wave-handling apparatus the characteristics of which are to be measured, and a cathode-ray oscilloscope having a recurrent sweep circuit and coupled to the output of said wave-handling apparatus, and a circuit coupling said second series of synchronizing pips to said sweep circuit for maintaining a stabilized visual presentation on said oscilloscope.

DONALD E. MAXWELL.

References Cited in the file of this patent UNITED STATES PATENTS Number Name Date 2,094,472 Rohats Sept. 28, 1937 2,189,457 Archer Feb. 6, 1940 2,280,226 Firestone Apr. 21, 1942 2,292,136 Lindsay et al Aug. 4, 1942 2,297,393 Deserno Sept. 29, 1942 2,310,342 Artzt Feb. 9, 1943 2,394,933 Mueller et a1 Feb. 12, 1946 2,443,603 Crost June 22, 1948 2,462,897 Rector Mar. 1, 1949 2,471,268 Gaines May 24, 1949 OTHER REFERENCES Williams: Radio News, January 1944, pages 24,

Moritz: Electronics, June 1946, pages -135. 

